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Phys. Rev. B 78, 144202 (2008) [7 pages]

Effect of local dipole moments on the structure and lattice dynamics of K0.98Li0.02TaO3

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Jinsheng Wen1,2,*, Guangyong Xu1, C. Stock3,4,†, P. M. Gehring4, Z. Zhong5, L. A. Boatner6, E. L. Venturini7, and G. A. Samara7
1Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA
2Department of Materials Science and Engineering, Stony Brook University, Stony Brook, New York 11794, USA
3Physics Department, The Johns Hopkins University, Baltimore, Maryland 21218, USA
4NIST Center for Neutron Research, National Institute of Standards and Technology, Gaithersburg, Maryland 20899, USA
5National Synchrotron Light Source, Brookhaven National Laboratory, Upton, New York 11973, USA
6Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
7Sandia National Laboratories, Albuquerque, New Mexico 87185, USA

Received 2 July 2008; revised 4 September 2008; published 8 October 2008

We present high-energy x-ray (67 keV) and neutron-scattering measurements on a single crystal of K1−xLixTaO3 for which the Li content (x=0.02) is less than xc=0.022, the critical value below which no structural phase transitions have been reported in zero field. While the crystal lattice does remain cubic down to T=10 K under both zero-field and field-cooled (E≤4 kV/cm) conditions, the Bragg peak intensity changes significantly at TC=63 K. A strong and frequency-dependent dielectric permittivity is observed at ambient pressure, a defining characteristic of relaxors. However an extensive search for static polar nanoregions, which is also widely associated with relaxor materials, detected no evidence of elastic neutron diffuse scattering between 300 and 10 K. Neutron inelastic scattering methods were used to characterize the transverse acoustic and optic phonons (TA and TO modes) near the (200) and (002) Bragg peaks. The zone-center TO mode softens monotonically with cooling but never reaches zero energy in either zero field or in external electric fields of up to 4 kV/cm. These results are consistent with the behavior expected for a dipolar glass in which the local polar moments are frozen and exhibit no long-range order at low temperatures.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.78.144202
DOI:
10.1103/PhysRevB.78.144202
PACS:
61.05.fg, 61.05.cf, 77.80.Dj, 77.84.Dy

*Corresponding author. jwen@bnl.gov

Also at ISIS, Rutherford Appleton Laboratory, UK.